• Journal of the Korean Solar Energy Society
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• v.26 no.4
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• pp.55-61
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• 2006

Titanium oxide ($TiO_2$) films are deposited on the indium tin oxide (ITO) substrate in an $Ar/O_2$ atmosphere by using reactive RF (Radio Frequency) magnetron sputtering technique, and Electrochromic properties and durability of $TiO_2$ films deposited at different preparation conditions are investigated by using UV-VIS spectrophotometer and cyclic voltammetry Li+ interalation/deintercalation in $TiO_2$ films shows that the electrochromic properties and durability of as-deposited films strongly depend on gas pressure $TiO_2$ films formed in our sputtering conditions are found to remain transparent, irrespective of their Li+ ion contents. The optimum sputtering conditions for film as passive counter electrode in electrochromic devices are working pressure of $1.0\;{\times}\;10^{-2}\;torr$ and oxygen flow raes of $10{\sim}15\;sccm$, respectively.

• Proceedings of the Materials Research Society of Korea Conference
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• 2011.10a
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• pp.22.1-22.1
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• 2011

In this study, off-axis RF magnetron sputtering was used for the crystallized ITO thin films at a low temperature of about $120^{\circ}C$ instead of the conventional RF sputtering because the off-axis sputtering can avoid the damage for the plasma as well as fabrication of thin films with a high quality. The structural, optical and electrical properties of the obtained films depending on deposition parameters, such as sputtering power, gas flow and working pressure, have been investigated. The ITO thin films grown on PET substrate at $120^{\circ}C$ were crystallized with a (222) preferred orientation. 100-nm thick ITO films showed a resistivity of about $4.2{\times}10^{-4}{\Omega}-cm$ and a transmittance of about 81% at a wavelength of 550nm. The transmittance of the ITO thin films by an insertion of $SiO_2$ thin films on ITO films was improved.

• Korean Journal of Materials Research
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• v.26 no.12
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• pp.676-680
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• 2016

We have investigated the properties of thin film transistors(TFT) fabricated using zinc tin oxide(ZTO) thin films deposited via on-axis sputtering and FTS methods. ZTO thin films deposited by FTS showed lower root-mean-square(RMS) roughness and more uniformity than those deposited via on-axis sputtering. We observed enhanced electrical properties of ZTO TFT deposited via FTS. The ZTO films were deposited at room temperature via on-axis sputtering and FTS. The as-deposited ZTO films were annealed at $400^{\circ}C$. The TFT using the ZTO films deposited via FTS process exhibited a high mobility of $12.91cm^2/V.s$, a low swing of 0.80 V/decade, $V_{th}$ of 5.78 V, and a high $I_{on/off}$ ratio of $2.52{\times}10^6$.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.234-234
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• 2011

IGZO 투명 전도 박막은 TFT-LCD에 사용되는 투명 전도성 산화물 박막으로서 다양한 광전자 소자의 투명 전극으로 널리 사용되고 있다. 본 연구에서는 RF magnetron sputtering법으로 corning 1737 유리기판 위에 RF 파워의 변화에 따라 증착한 IGZO박막의 광학적 전기적 특성 변화를 연구하였다. 박막 증착 조건은 초기 압력 $2.0{\times}10^{-6}$ Torr, 증착 압력 $2.0{\times}10^{-2}$ Torr, 반응가스 Ar 50 sccm, 증착 온도는 실온으로 고정하였으며, 공정변수로 RF 파워를 25 w, 50 w, 75 w, 100 w로 변화시키며, IGZO 타겟은 $In_2O_3$, $Ga_2O_3$, ZnO 분말을 각각 1 : 1 : 2 mol% 조성비로 혼합하여 소결한 타겟을 사용하였다. 표면분석(AFM)결과 RF 파워가 증가함에 따라 거칠기가 증가하였으며, XRD 분석결과 Bragg's 법칙을 만족하는 피크가 나타나지 않는 비정질 구조임을 확인할 수 있었다. 가시광 영역에서 (450 nm~700 nm) 25 w일 때 85% 이상을 확인하였고, RF 파워가 증가할수록 밴드갭이 감소하는 것을 확인하였다. RF 파워가 100 w인 경우 carrier 밀도는 $7.0{\times}10^{19}\;cm^{-3}$, Mobility 13.4 $cm^2$/V-s, Resistivity $6.0{\times}10^{-3}\;{\Omega}-cm$로 투명전도막의 특성을 보였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.194-194
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• 2010

태양전지용 투명전도막에 사용되는 Al-doped ZnO (AZO) 막은 저가이면서도 가시광역 영역에서 갖는 우수한 투과율과 낮은 비저항을 갖는 특성 때문에 ITO의 대체 재료로서 최근 활발한 연구가 진행되고 있다. 특히, 양산 현장에서는 in-line type의 대형 sputtering system에서 증착하고 있으며 높은 증착 속도와 박막 특성의 균일도가 중요한 과제다. 본 연구에서는 $2\;m\;{\times}\;1\;m\;{\times}\;0.2\;m$의 sputtering system에서 기판 캐리어를 이용해서 커다란 기판을 좁고 긴 타겟의 양쪽으로 왕복 운동을 하는 swing dynamic deposition 방법으로 $272\;mm\;{\times}\;500\;mm$ 크기의 AZO target (Al 2 wt%)을 이용하여 bipolar pulsed dc로 증착하였다. 이 시스템의 배기는 TMP와 cryo pump를 이용해서 $5\;{\times}\;10^{-7}\;Torr$의 기본 진공도를 얻으며, 공정 중에는 TMP만 사용하였다. 하지만, 본 시스템의 TMP는 비대칭 적으로 한쪽에 치우쳐 설치되어 있는데, 이것이 챔버 내에서 공정 가스인 Ar의 유동의 불균일도를 초래하게 되며, 그것이 증착되는 박막의 두께 균일도 및 특성 균일도에 영향을 주고 있음을 알 수 있었다. 본 연구에서는 다른 기본 진공도에서 증착된 AZO 박막의 특성 차이를 알아보고 비대칭 배기 구조가 in-line type 시스템에서 어떠한 두께 및 특성 불균일도를 가져오는지, 그리고 시스템 내부에 발생시키는 압력 불균일도를 상용 3차원 전산 유체해석 프로그램인 CFD-ACE+를 이용하여 분석하였다.

• Journal of the Korean Magnetics Society
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• v.10 no.5
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• pp.232-236
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• 2000

CoSm thin films with a Cr underlayer have received continuous attention as a potential material for a high density longitudinal magnetic recording media. In this study the Ax gas sputtering pressure effects on the magnetic properties of CoSm thin films, which were fabricated by using a dc magnetron sputtering machine, were investigated. The magnetic switching volume is especially important parameter to understand the thermal stability of the written information, magnetization reversal process and media noise. Therefore, in this paper the effects of sputtering pressure on the magnetic switching volume of CoSm thin films grown on Cr underlayer with the same sputtering conditions was studied. As the Ar sputtering pressure during sputtering of the CoSm magnetic layer increases from 5 to 30 mTorr, the measured switching volumes decreased from 9.0 to 5.2$\times$10$^{-18}$ cm$^3$. The calculated diameter of switching unit from V＊ was less than 22 nm, which satisfies the Sharrock's requirement on the thermal stability of the high density longitudinal magnetic recording media.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2008.11a
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• pp.23-24
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• 2008

Bipolar pulsed dc magnetron sputtering을 이용하여 태양전지의 투명 전도막용으로 유리기판 위에 Al doped ZnO (AZO) 박막을 증착하였다. $400{\times}400\;mm$의 대면적 기판에 증착하기 위해서 $5{\times}25$ inch 대형 사각 AZO target (Al 2 wt%)을 사용했고, $50{\sim}250\;kHz$의 bipolar pulse를 인가하였다. 실제로는 $400{\times}400\;mm$ 면적의 기판에 slide glass 16개를 사용했으며, 약 700 nm 두께에서 두께와 투과도, 비저항의 균일도를 평가하였다. Bipolar pulse의 주파수 150 kHz일 때, 가장 우수한 특성을 갖는 AZO가 증착되었으며, $2.13{\times}10^{-3}{\Omega}{\cdot}cm$의 비저항에 가시광선 영역에서 82%의 투과율을 보였다. 또한, $400{\times}400\;mm$ 대면적 기판에서의 두께와 투과도, 비저항의 불균일도는 각각 5%, 1%, 9% 였다.

• Solar Energy
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• v.20 no.2
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• pp.55-65
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• 2000

Better electrical and optical properties of ITO thin films were demanded for the window layer of CdS/CdTe solar cells. To match that demand, an ion beam sputtering system was used for the deposition of ITO thin films. The substrate temperature and ion beam energy were controlled to deposit high quality ITO thin films in two cases of Ar ion sputtering and Ar+$O_2$ ion sputtering. The microstructure changed from domain structure in ITO deposited by Ar ions to grain structure in ITO deposited by Ar+$O_2$ ions. The lowest resistivity of ITO films was $1.5\times10^{-4}{\Omega}cm$ at $100^{\circ}C$ substrate temperature in case of Ar ions sputtering. Transmittance in the visible range was over 80% above $100^{\circ}C$ substrate temperature.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2003.07b
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• pp.787-790
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• 2003

A rf triode magnetron sputtering system is designed and installed its construction in vacuum chamber. In order to calibrate the rf triode magnetron sputtering for thin films deposition processes, the effects of different glow discharge conditions were investigated in terms of the deposition rate measurements. The basic parameters for calibrating experiment in this sputtering system are rf power input, gas pressure, plasma current, and target-to-substrate distance. Because a knowledge of the deposition rate is necessary to control film thickness and to evaluate optimal conditions which are an important consideration in preparing better thin films, the deposition rates of copper as a testing material under the various sputtering conditions are investigated. Furthermore, a triode sputtering system designed in our team is simulated by the SIMION program. As a result, it is sure that the simulation of electron trajectories in the sputtering system is confined directly above the target surface by the force of $E{\times}B$ field. Finally, some teats with the above 4 different sputtering conditions demonstrate that the deposition rate of rf triode magnetron sputtering is relatively higher than that of the conventional sputtering system. This means that the higher deposition rate is probably caused by a high ion density in the triode and magnetron system. The erosion area of target surface bombarded by Ar ion is sputtered widely on the whole target except on both magnet sides. Therefore, the designed rf triode magnetron sputtering is a powerful deposition system.

• Journal of the Korean Vacuum Society
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• v.9 no.2
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• pp.136-143
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• 2000

$SrBi_2Ta_2O_9;(SBT)$ films were deposited on p-type Si(100) at room temperature by rf magnetron sputtering method to confirm the possibility of application of $Pt/SBT/Pt/Ti/SiO_2/Si$ structure (MFM) for destructive read out ferroelectric RAM (random access memory). Their structural characteristics with the various annealing times and Ar/$O_2$ gas flow ratios in sputtering were observed by XRD (X-ray diffractometer) and the surface morphologies were observed by FE-SEM (field emission scanning electron microscopy), and their electrical properties were observed by P-V (polarization-voltage measurement) and I-V (current-voltage measurement). The Ar/$O_2$ gas flow ratios of sputtering gas were changed from 1 : 4 to 4 : 1 and SBT thin films were deposited at room temperature. The films show (105), (110) peaks of SBT by XRD measurement. SBT thin films deposited at room temperature were crystallized by furnace annealing at 80$0^{\circ}C$ in oxygen atmosphere during either one hour or two hours. Among their electrical properties, P-V curves showed shaped hysteresis curves, but the SBT thin films showed the asymmetric ferroelectric properties in P-V curves. When Ar/$O_2$ gas flow ratios are 1 : 1, 2: 1, the leakage current density values of SBT thin films are good, those values of 3 V, 5 V, and 7 V are respectively $3.11\times10^{-8} \textrm{A/cm}^2$, $5\times10^{-8}\textrm{A/cm}^2$, $7\times10^{-8}\textrm{A/cm}^2$.After two hours of annealing time, their electrical properties and crystallization are improved.